Sound processor for a cochlear implant

ABSTRACT

The sound processor and method uses a model of basilar membrane motion to select stimuli, based upon the predicted motion which the acoustic signal presented would produce in an acoustically excited normally hearing cochlea. The filter; used, in contrast to single channel per electrode approaches, cover multiple channels and overlap with each other. Consequently the stimuli presented produce a neural excitation pattern which approximates the spatio-temporal travelling wave observed on the basilar membrane in an acoustically excited normally hearing cochlea. Preferably, the predicted electrode stimuli are based upon the instantaneous predicted amplitude of the electrode location.

TECHNICAL FIELD

The present invention relates to cochlear implants, and to sound processing devices and methods relating to cochlear implants.

BACKGROUND ART

In normal hearing, sound causes mechanical vibrations that stimulate the hair cells of the cochlea to produce electrical impulses that travel down the auditory nerve where they are perceived by the brain as sound. If for some reason these hair cells are destroyed or not present within the cochlea, as is the case with individuals with severe or profound hearing loss, the nerve cells do not receive this electrical stimulation, therefore no sound is perceived. A cochlear implant attempts to replace this lost function by providing artificial electrical stimulation of the surviving auditory nerve. Cochlear implants have been in clinical use for many years. Such devices use an array of implanted electrodes to provide electrical stimuli to the cochlea. The electrical stimuli are determined by a processor responsive to speech and sound signals in the environment of the user.

Historically, prior to around 1994, the majority of speech processors used in conjunction with a cochlear implant employed speech processing strategies that can be described as Feature Extraction Strategies. In such strategies, the associated implant hardware attempts to identify the speech features present in the detected sound signal and encodes such features as patterns of electrical stimulation. Feature extraction strategies have the advantage that the hardware required to perform the feature extraction is relatively simple and consumes a relatively low amount of power.

With improvements in silicon chip technology and an increased knowledge of the safety of electrical stimulation, a new approach in sound processing became possible. This approach had the ability to provide a full range of spectral information of the speech signal without the need for the hardware to fit the signal into a preconceived mould, giving the patient the opportunity to listen to the particular information of interest, within background noise, providing a more realistic approach to speech processing. Such sound processors use band-pass filters to separate acoustic signals into frequency bands or spectral components with relatively little overlap of the bands, with the electrodes being stimulated in a tonotopic fashion according to the energy in those bands. Usually they present a smoothed (low-pass-filtered) representation of the amplitude from each band to a single electrode.

Despite considerable practical success with each of the existing schemes, the user perceptions of existing devices indicate that there are significant outstanding problems. Three fundamental problems of sound perception reported by cochlear implant users are poor frequency resolution and discrimination, poor perception of speech in noise at low signal-to-noise ratios, and poor perception of musical sounds.

It is an object of the present invention to provide an alternative speech processor and processing method, in order to further improve the practical performance of the cochlear implant system.

SUMMARY OF THE INVENTION

In broad terms, the present invention provides a fundamental change to the traditional approach used in sound processing for cochlear implants. Instead of attempting to separate acoustic information into discrete frequency bands or channels, the inventive processor produces electrical stimulation patterns that excite broad overlapping regions of the cochlea. It is believed that the approach of the present invention will provide a better approximation to the behavior of the auditory structures during hearing by a normally hearing listener. Current processors produce localised stimuli based upon the frequency of components of the sound signal. In contrast, the present invention seeks to approximate the spatio-temporal neural excitation patterns which are induced by the motion of the basilar membrane as a response to sound stimuli in the normally hearing listener. The present invention seeks to produce a spatio-temporal pattern of stimulation along the length of an intra-cochlea electrode array, as opposed to merely localised stimuli.

According to a first aspect, the present invention resides in a method of processing sound signals in order to generate electrical stimuli for an auditory prosthesis whereby a neural excitation pattern is produced which mimics the spatio-temporal pattern associated with the travelling wave observed on the basilar membrane in an acoustically excited normally-hearing cochlea.

According to another aspect, the present invention provides a sound processor for use in a cochlear implant system, said sound processor being of the type which receives sound signals from a microphone or the like, processes said signals according to a predetermined instruction set, and provides stimulation instructions for an implanted electrode array, characterised in that the predetermined instruction set produces stimulus instructions which are intended to provide an approximation to the spatio-temporal waveforms induced in response to said sound signals on the basilar membrane of a normal hearing listener.

According to yet another aspect, the present invention provides a method of processing sound signals so as to produce stimulus instructions for a cochlear implant, including the steps of deriving the vector of complex Fourier transform coefficients for a data sample;

multiplying the vector of the coefficients by a complex matrix representing the amplitude and phase of the Fourier frequency components at the position of the electrodes in the cochlea relative to the amplitude and phase at the stapes in a normal cochlea to produce an output vector; and

converting the output vector values to electrode current levels.

Travelling wave aspects of basilar membrane response have been observed and reported on in investigations of normal auditory processes. However, there has been no previous attempt to utilise these phenomena as an element of stimulus processing for cochlear implants. The travelling wave may be thought of as a 3-Dimensional pattern in which the dimensions are time, distance along the basilar membrane, and displacement of the basilar membrane. The properties of these patterns that are thought to be important (and different from existing processor outputs) include a diagonal ridge structure of the 3D pattern, the dynamic nature of the ridge pattern that sweeps across the cochlear electrode array at a particular velocity that depends on position, the smoothly varying nature of the pattern in both space and time, and the maintenance of naturally-occurring phase and amplitude relationships between the stimulation patterns on individual electrodes.

BRIEF DESCRIPTION OF DRAWINGS

The implementation of the present invention will be described in more detail with reference to the accompanying drawings, in which:

FIG. 1 is a graph illustrating a travelling wave excitation pattern produced in response to a pure tone of frequency 200 Hz;

FIG. 2 is a graph illustrating a travelling wave excitation pattern for tones at 200 and 600 Hz;

FIG. 3 is a graph illustrating a travelling wave excitation pattern for tones at 470 and 200 Hz;

FIG. 4 is a schematic illustration of one implementation of the invention;

FIG. 5 is a block diagram of one speech processing implementation of the present invention;

FIG. 6 is a graph of the typical frequency response of a 22-channel filterbank;

FIG. 7 is a graph depicting the typical delay of each of each of the 22 channels;

FIG. 8 is a block diagram showing the sub-components of the Electrical Encoding Component of FIG. 5.

DETAILED DESCRIPTION

The present invention will be described with reference to the hardware implementation used by the applicant, using an implanted receiver/stimulator unit and an external speech processor and microphone. However, the present invention is of broad scope and can be implemented on any sufficiently sophisticated cochlear implant system. In particular, it is anticipated that the present invention will be able to be implemented more fully and in more detail on future generations of cochlear implants, with increased processing power and flexibility relative to the current state of the art. The present invention could also be implemented in a totally implanted device, or some intermediate stage between the present systems and a totally implanted device.

The essential difference between the invention described and previous implant coding schemes is that the importance of overlapping information across electrodes is recognized and a complex spatio-temporal pattern is produced. This pattern preserves, at least in part, the detailed amplitude and phase relationships between different positions that occur normally in an intact cochlea. These amplitude and phase relationships vary smoothly as a function of position along the cochlea to produce the acoustic “travelling wave” (von Bekesy, 1961). Instead of attempting to separate acoustic information into discrete frequency bands or channels, the travelling wave processor produces electrical stimulation patterns that excite broad overlapping regions of the cochlea. As an example, FIG. 1 shows the excitation pattern that is produced by the inventive travelling wave processor in response to a pure tone input signal. Each line in FIG. 1 shows the shape of the excitation function at an instant in time. The horizontal axis represents position along the cochlea from the basal (high frequency) end on the left to the apical (low frequency) end on the right.

In contrast, the excitation pattern produced by the same pure tone input signal after processing by any of the currently used cochlear implant coding schemes would be localized to one position in the cochlea and represented by a narrow ridge running vertically up the page in a Figure analogous to FIG. 1. In some cochlear implant coding schemes the amplitude of the vertical ridge would be represented by electrical pulses at a fixed rate and level (ACE, SPEAK), or modulated at a rate equal to the frequency of the (low-frequency) input tone (F0F2, F0F1F2, MPEAK, CIS, SAS). In the latter cases, the excitation pattern is effectively a vertical slice taken from the pattern of FIG. 1 at the point where the amplitude of the pattern is greatest.

It is hypothesized that the auditory pathways of the brain have specialized perceptual mechanisms designed to recognize characteristics of 3-dimensional (position ×time ×amplitude) excitation patterns like those shown in FIG. 1. It is known that the visual and tactile sensory systems have neural mechanisms specialized to detect the orientation and spacing of stripes and ridges. The auditory system may be programmed in an analogous manner to recognise the diagonal ridges of patterns like the one in FIG. 1. If an incomplete pattern is presented to the cochlea (as in all prior art cochlear implant coding schemes) these perceptual mechanisms will be engaged but will not operate as effectively as they would if the whole pattern was presented. It is hypothesized that the presentation of complete 3D patterns will improve the perception of sound by cochlear implant users and overcome or reduce some of the problems that are common to all prior art cochlear implant systems. Relative to normal hearing listeners, the problems for implant users include poor frequency discrimination and resolution abilities, poor speech recognition of speech in background noise, and lack of musical quality for processed musical sounds.

When the stimulation is viewed as a 3D pattern, several consequences become more apparent:

-   -   a) A whole pattern is easier to recognize than a partial pattern         because it contains more information. This characteristic is         also important for grouping sound components from the same         source. Some of the temporal and spatial coherence of excitation         patterns arising from a single sound source is lost when the         signal is band-pass filtered into separate components that are         encoded independently of one another. Conversely, sounds from         different sources will be easier to separate if each one gives         rise to a whole pattern, rather than a number of independent         components which must be recombined by the perceptual mechanisms         into an unknown number of sound sources. In the particular case         of speech in background noise, it is important that the speech         and the noise both produce complete 3D excitation patterns so         that the perceptual mechanisms can use this information to         allocate components of the combined pattern more easily to the         noise or to the speech.     -   b) Dynamic patterns are easier to recognise than stationary         ones. It is well-known that the tactile system provides         increased information about texture, shape and edges of objects         if the fingers are moved over the surface of the object than if         a static contact is made. In a similar way, the spacing of         ridges in the 3D auditory excitation pattern may be enhanced         perceptually by sweeping them along the cochlea. Similarly,         onsets and offsets of sounds correspond to edges in the 3D         pattern, and these may be perceived more clearly as they move         along the cochlea, rather than just appearing with different         amplitudes at different parts of the cochlea and then         disappearing again. Thus the presentation of dynamic patterns         may improve frequency discrimination and resolution and         perception of onsets and offsets of sounds with complex spectra.     -   c) If a pattern is known to vary smoothly and regularly, missing         sections can be interpolated or filled in. For example, one can         “see” what is on the other side of a paling fence as one walks         past even though most of the scene is obscured by the fence at         any one time. This is because the visual system is able to         reconstruct the continuous picture from the parts that are         viewed at separate instants in time. In the case of auditory         signals that are obscured by noise, parts of a smoothly varying,         regular speech pattern may be perceived through temporal and         spectral gaps in the noise and reconstructed in an analogous         manner. However, if the speech and noise patterns do not vary         smoothly with position, this reconstruction is much more         difficult. This is a potential explanation for the fact that         implant users are unable to recognize speech in noise when the         signal-to-noise ratio is close to zero. The travelling wave         processor may allow listeners to reconstruct lower amplitude         speech signals even when they are partially obscured by more         intense noise signals, provided that there are some temporal or         spectral gaps in the noise signal.     -   d) Tone complexes with harmonically related components produce         3D patterns with special characteristics in the regions where         the tonal patterns overlap. These characteristics are not         present in anharmonic complexes. They are also not present in         the excitation patterns produced by existing cochlear implant         sound processors because they do not produce overlapping         patterns for individual tones separated by an octave or more.         For example, FIG. 2 shows the excitation pattern for 2 tones at         200 and 600 Hz. In the overlap region, every third diagonal         ridge is larger than the others because of the constructive         addition of the two excitation patterns. FIG. 3 shows an         anharmonic combination where there is no regular summation of         the two patterns in the overlap region.

The travelling wave in normal hearing has been recognised and discussed in the scientific literature. However, this literature has had virtually no effect on the design of cochlear implants or hearing aids as far as the inventors are aware. One explanation for this is that the frequency response of the cochlea to sinusoidal signals is highly peaked and implant and hearing aid designers have chosen to ignore the low-frequency tails of the frequency response curves. The closest existing technologies are cochlear implant sound coding schemes that measure spectral characteristics of input signals with bandpass filters and represent them by stimulating individual electrodes.

The preferred implementation of the present invention utilizes a digital-signal-processor to calculate an approximate travelling wave excitation pattern from a digitised input signal. The travelling wave pattern is essentially a specification of the displacement of each point on the basilar membrane of the cochlea as a function of time and position. The implementation is based directly on published experimental data from normally-hearing human subjects rather than theoretical models of basilar membrane mechanics. The implementation is also simplified to make it feasible for real-time implementation and to make it easier to parameterize the fitting procedure for individual cochlear implant users.

One embodiment of the system according to the present invention is shown in FIG. 4, with the components of the system as listed below:

-   -   1. Microphone 11 to convert an acoustic input signal to an         electrical signal,     -   2. Preamplifier/Automatic Gain Control 12 to amplify and control         the level of the electrical signal.

3. Analog -to-Digitl-Converter 13 to convert the electrical signal to a stream of ditigal samples.

-   -   4. Digital-Signal-Processor 14 to calculate the travelling wave         pattern and convert it to an electrical stimulus pattern.     -   5. Programmable Memory 15 to store patient-specific parameters,         the processor programs, and intermediate results in calculating         the travelling-wave pattern.     -   6. Output Signal Generator 16 to control a cochlear implant and         deliver the electrical stimulus to the implant patient.

A simpler version of the present invention, in particular the digital signal processor, is shown in FIG. 5. In this particular aspect, the invention essentially resides in a system consisting of four main parts: a Basilar Membrane Motion Model which accepts an audio signal as input and calculates the displacement or velocity of the basilar membrane at each electrode position; an Inner Hair Cell Model which calculates the amount of neural excitation at each electrode position based on the information received from the Basilar Membrane Motion Model; an Outer Hair Cell Model which provides a feedback path that takes into consideration the amount of neural excitation calculated by the Inner Hair Cell Model and the effects such excitation will have on the Basilar Membrane Motion Model whereby the amount of neural excitation affects the response of the Basilar Membrane Motion Model; and an Electrical Encoding Component which calculates the pattern of electrical stimulation which will provide the desired neural excitation pattern. Each of these 4 components will be described in more detail below. velocity of the basilar membrane at each electrode position; an Inner Hair Cell Model which calculates the amount of neural excitation at each electrode position based on the information received from the Basilar Membrane Motion Model; an Outer Hair Cell Model which provides a feedback path that takes into consideration the amount of neural excitation calculated by the Inner Hair Cell Model and the affects such excitation will have on the Basilar Membrane Motion Model; whereby the amount of neural excitation affects the response of the Basilar Membrane Motion Model; and an Electrical Encoding Component which calculates the pattern of electrical stimulation which will provide the desired neural excitation pattern. Each of these 4 components will be described in more detail below.

Basilar Membrane Motion Model

The Basilar Membrane Motion Model accepts an audio signal as input and calculates the displacement or velocity of the basilar membrane at each electrode position in relation to the audio signal.

One possible embodiment of the Basilar Membrane Motion Model consists of the following steps, which are repeated continuously:

-   -   1 The input audio signal is divided into short overlapping         frames. Each frame contains L consecutive samples of the audio         signal, and is defined as the column vector X1. A suitable         length is L=128. Each frame heavily overlaps with the previous         frame, and contains K new data points. A suitable value is K=1.     -   2 Multiply the input frame vector X1 point-by-point by a window         vector W, resulting in a column vector X2 of length L, according         to:         X 2(n)=X 1(n)*W(n) for n=0 to L−1.     -   A suitable window function is the Hann function, defined as:         W(n)=0.5*(1−cos(2*n*pi/L)) for n=0 to L−1.     -   3 Calculate the L-point Fast Fourier Transform (FFT) of the         column vector X2. This results in a column vector X3 of length         L, with complex values. Because X2 is real, X3 has Hermitian         symmetry, and the last L/2 samples can be discarded (or not         calculated). From the first L/2 samples, only the real parts are         required and the imaginary parts are discarded (or not         calculated). The output is a real column vector X4 of length         L/2.     -   4 Multiply column vector X4 by a rectangular weights matrix G,         according to:         X 5 =G*X4.         The weights matrix G has N rows and L/2 columns. The output is a         column vector X5 of length N, where N is the number of channels.         The weights matrix G determines the frequency magnitude response         of each channel, and is further described below.     -   5 Delay each channel by a time delay specified by column vector         D, which has length N, according to the formula:         X 6(k, t)=X 5(k, t−D(k)) for k=1 to N

Typical delays for a 22-channel processor are shown in FIG. 7. The delay varies from zero delay at channel 1 (the most basal channel) to 8 milliseconds at channel 22 (the most apical channel).

The output is a column vector X6 of length N, where each element is a sample of one channel of the Basilar Membrane Motion Model.

Each row of the matrix W represents the amplitude and phase of the FFT frequency components at the position of one of the electrodes in the cochlea relative to the amplitude and phase at the stapes (the input to the cochlea). The phase difference is equal to 2 pi times the time taken for the travelling wave to travel from the stapes to the position of the electrode multiplied by the frequency of the FFT component. The amplitude difference between the stapes and the electrode position is proportional to the response of the basilar membrane at the position of the electrode to a pure tone at the frequency of the FFT component (or alternatively, the tuning curve of a neuron at the position of the electrode). The amplitude coefficients at each electrode position have a peaked shape with the maximum at the FFT frequency closest to the characteristic frequency at the individual electrode position, and the amplitudes of FFT coefficients higher than this frequency fall rapidly to zero.

An alternative way of implementing the delays in this system is by shifting the FFT window back in time by a different amount for each electrode. If the shift is chosen to be equal to the time taken for the travelling wave to travel from the stapes to the electrode position, then the coefficients of the matrix W are all real (ie the phase is zero for all FFT components).

The weights matrix G can be calculated according to the following steps:

-   -   1. The characteristic frequency of each channel is determined         based on the position of the electrodes in the cochlea,         according to Greenwood's formula. A further correction should be         applied to account for the fact that electrodes at a particular         position in the cochlea actually stimulate neurons with a lower         characteristic frequency than that predicted by Greenwood's         formula (Blarney P J, Dooley G J, Parisi E S and Clark G M.,         “Pitch comparisons of acoustically and electrically evoked         auditory sensations”. Hearing Research 99 139–150, 1996; James         C, Blarney P J, Shallop J K, Incerti P V & Nicholas A M.         “Contralateral masking in cochlear implant users with residual         hearing in the non-implanted ear”, Audiology and Neuro-Otology,         6, 87–97, 2001). This correction factor implies that the         effective distance of the electrode from the stapes is greater         by a factor of 2.625/1.875. Alternatively, for subjects who have         previously used another sound processor and have become         accustomed to a particular frequency-to-electrode map, those         frequencies can be used. The characteristic frequencies are         stored in a vector C of length N.     -   2. The centre frequency of each FFT bin is calculated and stored         in vector B, of length L/2.     -   3. The weights matrix element G(k, b) represents the gain of         channel k at the centre frequency of FFT bin b, and can be         calculated according to the formula:         if B(b)<=C(k)         G(k, b)={B(b)/C(k)}^E         else         G(k, b)=0     -   where the symbol “^” means “to the power of” and the parameter E         is called the gain exponent. Suitable values for E are in the         range 1 to 5. Suitable choices for characteristic frequencies         for 22 channels, with a gain exponent E=1 result in the         magnitude response shown in FIG. 6.

The amplitude of each FFT component at each electrode position is represented by the magnitude of the corresponding element in matrix W. These amplitudes may be estimated from psychophysical tuning curves in humans with normal hearing (Zwicker, E. “On a psychophysical equivalent of tuning curves.” In Zwicker E. & Terhardt E (eds) Facts and models in hearing. pp132–141, Berlin: Springer-Verlag, 1974), from estimates of excitation in the loudness models of Zwicker (Zwicker E. “Masking and psychological excitation as consequences of the ear's frequency analysis,” in Plomp R & Smoorenburg GF (Eds) Frequency analysis and periodicity detection in hearing, pp376–96, Leiden: AW Sijthoff, 1970) or Moore & Glasberg (Moore BCJ & Glasberg BR. A model of loudness perception applied to cochlear hearing loss. Auditory Neuroscience 3, 289–311, 1997) or from an approximation or from an empirical function designed to optimise the travelling wave processor for individual implant users.

Inner Hair Cell Model

The Inner Hair Cell Model calculates the amount of neural excitation at each electrode position based on the displacement or velocity of the basilar membrane at each electrode position in relation to the audio signal as calculated by the Basilar Membrane Motion Model as discussed above. A simple embodiment of the Inner Hair Cell Model is a half-wave rectifier, with other embodiments possible as would be obvious to those skilled in the art. The half wave rectification mimics the response of the hair cells in a normal cochlea. The amplitude of the half-wave rectified travelling wave at each electrode position is represented by the current level (or electric charge, or pulse width) of an electric pulse on that electrode. This mapping from amplitude to electrical stimulation parameters differs from conventional cochlear implant mapping in that the instantaneous amplitude of the travelling wave is represented rather than a smoothed amplitude or intensity which is averaged over a time window of several milliseconds. Conventional processors code the amplitude envelope rather than the instantaneous amplitude, and in doing so, they lose much of the temporal information carried by the signal itself. The coding of instantaneous amplitude is especially important to the travelling wave processor because coding envelope information would merely smear out the information from different frequency components rather than providing the detailed timing information illustrated in FIGS. 1–3. In particular the 3-dimensional ridges would become much broader in both spatial and temporal dimensions, and would lose their dynamic characteristics.

Outer Hair Cell Model

The Outer Hair Cell model aims to emulate the non-linearity that is observed in the response of a person with normal hearing. This is performed by providing a feedback path to the Basilar Membrane Motion Model which takes into consideration the proposed neural excitation pattern and the affects such a pattern has on the response of the Basilar Membrane Motion Model. The output of the Inner Hair Cell Model is an estimate of the neural excitation pattern that would be present in a person with normal hearing. It has been found that the gain for low-amplitude audio signals is greater than the gain for large-amplitude audio signals. This component is optional and may be omitted in a simplified implementation.

Electrical Encoding Component

The Electrical Encoding component calculates the pattern of electrical stimulation that will provide the desired neural excitation pattern. There are several possible embodiments of the Electrical Encoding component and some components that are used in the prior art of cochlear implant processors can be used to perform this function according to the present invention. It is important to note that it is the instantaneous amplitude of the waveform at each electrode position which is coded as the current level (or electric charge or pulse width) of an electric pulse on that electrode. This differs greatly from prior art systems where it is the time-averaged amplitude envelope of the waveform which constitutes what is coded as the current level of an electric pulse on that electrode. In essence, the conversion is effected by means of a function relating the amplitude to electric current level derived from prior measurements for each electrode which may be stored in the memory 15.

The present invention can be used with implants that allow both simultaneous and/or non-simultaneous stimulation. If the invention is used on an implant that stimulates channels simultaneously, the travelling wave amplitudes at individual electrode positions can be represented by simultaneous electric currents (analog rather than pulsatile stimuli) on each individual electrodes.

If the invention is used with an implant that stimulates channels sequentially (non-simultaneously), then the Electrical Encoding component can be divided into two sub-components as illustrated in FIG. 8. The Sampler component samples the neural excitation pattern such that each output sample produces one electrical pulse. The Amplitude Mapping component calculates the electrical parameters of the pulse, such as current level and pulse width.

One simple embodiment of the Sampler component is taken from the well known Continuous Interleaved Sampling (CIS) processor. The neural excitation pattern is sampled in a round-robin fashion at a uniform rate on each channel, so the sampling rate is equal to the stimulation rate on each channel. The samples are interleaved across channels so that the electrical pulses are sequential (non-overlapping). The rate must be sufficiently high so that the time waveform of the neural excitation on each channel is adequately represented. Typically this requires more than 1000 pulses per second on each channel.

Note that in a standard CIS processor the filters are designed to be non-overlapping and relatively narrow, and the smoothed envelope of the filter outputs are sampled. In contrast, the present invention has broad, heavily overlapping filters and the instantaneous amplitude of the half-wave rectified filter output is sampled.

The CIS Sampler embodiment has the disadvantage that high stimulation rates are required. An alternative embodiment, which is new in this invention, is called the Time Interval Maxima Sampler. It reduces the total stimulation rate that is required. It has the following steps:

-   -   1. The neural excitation pattern is divided into short         non-overlapping time intervals. Each time interval can be         represented as a matrix X that has N columns, where N is the         number of channels, and T rows, where T is the number of time         samples of the neural excitation pattern in each time interval.         The duration of the time interval is equal to the time taken to         output a number M of electrical pulses, where M is less N.     -   2. In each time interval the maximum value of each channel is         calculated, i.e. the maximum of the matrix X across the rows.         The output is a column vector Y with N columns, one for each         channel.     -   3. The amplitudes of the N samples in column vector Y are         examined, and the M largest samples are retained. Each of these         M samples produces one electrical pulse. The pulses are output         in the next time interval.

The Amplitude Mapping component can be the same as that used in the prior art Continuous Interleaved Sampling (CIS) processor or Spectral Maxima Sound Processor (SMSP). It has the following steps:

-   -   1. The amplitude of each sample is compressed by a non-linear         function known as a loudness growth function, which typically         has a logarithmic shape. Each output P represents a proportion         of the electrical dynamic range.     -   2. The current level L of each electrical pulse is calculated         from the output P and the previously measured threshold T and         maximum comfortable level C (for that channel) as:         L=T+(C−T)*P

Following this, the electrode(s) to be stimulated are selected, and the output signal generator 16 is fed the data required to produce the electrical stimulus pulses.

It will be appreciated that there are various ways of implementing the present invention, for example using circuitry to provide the travelling wave type stimuli, which are included within the scope of the present inventive concept. Variations and additions are also possible within the general inventive concept disclosed. 

1. A method for generating electrical stimuli in an auditory prosthesis an implanted electrode array having a plurality of electrodes representing received sound signals, comprising: processing the sound signals according to a predetermined instruction set that calculates a travelling wave amplitude variation at each electrode position using broad overlapping filters, comprising: sampling said sound signals to produce a data sample; deriving a vector of complex Fourier transform coefficients for said data sample; and multiplying the vector of the coefficients by a complex matrix representing an amplitude and phase of the Fourier frequency components at said each electrode position in a damaged cochlea relative to an amplitude and phase at the stapes in a normal cochlea to produce an output vector; converting said output vector to a set of stimulus instructions for said electrode array; and wherein said filters are not specific only to the frequencies associated with said each electrode position of said electrode array.
 2. The method of claim 1, further comprising: adjusting a group delay of said filters to account for the time for an acoustic signal takes to propagate from the stapes to said each electrode position in an acoustically excited normally-hearing cochlea.
 3. The method of claim 1, wherein said travelling wave amplitude is based on an instantaneous amplitude of said sound signal.
 4. The method according to claim 1, further comprising: providing said electrical stimuli on said electrode when said travelling wave at said each electrode position reaches a local maximum.
 5. The method according to claim 4, further comprising: stimulating said electrode position having the larger amplitude value first when said travelling wave at more than one of said each electrode positions reaches said local maximum at the same time.
 6. A method of processing sound signals for use in an auditory prosthesis implant, comprising: sampling said sound signals to produce digital data samples; calculating a traveling wave excitation pattern using digital data samples based on the amplitude and phase at each electrode position in a damaged cochlea relative to the amplitude and phase at the stapes in a normal cochlea; and converting said traveling wave excitation pattern to a set of stimulus instructions.
 7. The method of claim 6, further comprising: calculating the amount of neural excitation at said each electrode position.
 8. The method of claim 7, further comprising: providing a feedback path from said calculating the amount step to said calculating said pattern step.
 9. The method of claim 6, said calculating step pattern step further comprises: deriving the vector of complex Fourier transform coefficients for said data sample; multiplying the vector of the coefficients by a complex matrix representing the amplitude and phase of the Fourier frequency components at said each electrode position in said damaged cochlea relative to the amplitude and phase at the stapes in said normal cochlea to produce an output vector; and converting the output vector to said set of stimulus instructions for an electrode array having a plurality of electrodes.
 10. A method of processing sound signals for use in generating electrical stimuli for an auditory prosthesis, said method comprising: processing said sound signals according to a predetermined instruction set, wherein said predetermined instruction set calculates a travelling wave amplitude variation at each electrode position using broad overlapping filters; and converting the output of said predetermined instruction set to a set of stimulus instructions for an implanted electrode array having a plurality of electrodes; wherein said filters are not specific only to the frequencies associated with said each electrode position of said electrode array, wherein said travelling wave amplitude is based on the instantaneous amplitude of said sound signal.
 11. A method of processing sound signals for use in generating electrical stimuli for an auditory prosthesis, comprising determining a phase and amplitude of said sound signal at each electrode position in an acoustically excited normally-hearing cochlea when stimulated with said sound signal using a basilar membrane model to produce a neural excitation pattern; and calculating a level of neural excitation at said each electrode position in said acoustically excited normally-hearing cochlea when stimulated with said sound signal using an inner ear model; wherein said neural excitation pattern approximates the spatio-temporal pattern associated with a travelling wave observed on the basilar membrane in said acoustically excited normally-hearing cochlea when stimulated with said sound signal.
 12. The method according to claim 11, wherein said inner hair cell model is a half-wave rectifier.
 13. The method according to claim 11, further comprising: feeding back the effect the response of said neural excitation pattern on the basilar membrane to said basilar membrane model using an outer hair cell model.
 14. The method according to claim 11, further comprising: encoding said neural excitation pattern to generate said electrical stimuli. 